SPS flanges Simulations & Measurements Update Fritz Caspers and Jose E. Varela.
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Transcript of SPS flanges Simulations & Measurements Update Fritz Caspers and Jose E. Varela.
![Page 1: SPS flanges Simulations & Measurements Update Fritz Caspers and Jose E. Varela.](https://reader037.fdocuments.net/reader037/viewer/2022100403/5a4d1af27f8b9ab05997ed44/html5/thumbnails/1.jpg)
SPS flangesSimulations & Measurements
Update
Fritz Caspers and Jose E. Varela
![Page 2: SPS flanges Simulations & Measurements Update Fritz Caspers and Jose E. Varela.](https://reader037.fdocuments.net/reader037/viewer/2022100403/5a4d1af27f8b9ab05997ed44/html5/thumbnails/2.jpg)
Outline
• Introduction• Impedance List Update• Damping Resistors in Simulations• Conclusions
![Page 3: SPS flanges Simulations & Measurements Update Fritz Caspers and Jose E. Varela.](https://reader037.fdocuments.net/reader037/viewer/2022100403/5a4d1af27f8b9ab05997ed44/html5/thumbnails/3.jpg)
Introduction• We continue to search for possible causes of the
suspected 1.4GHz microwave instability in the SPS.
• Last element of the list was simulated and impedance has been included in the table.
• Small study on the possibility of including the damping resistors in simulations has been carried out.
![Page 4: SPS flanges Simulations & Measurements Update Fritz Caspers and Jose E. Varela.](https://reader037.fdocuments.net/reader037/viewer/2022100403/5a4d1af27f8b9ab05997ed44/html5/thumbnails/4.jpg)
Outline
• Introduction• Impedance List Update• Damping Resistors in Simulations• Conclusions
![Page 5: SPS flanges Simulations & Measurements Update Fritz Caspers and Jose E. Varela.](https://reader037.fdocuments.net/reader037/viewer/2022100403/5a4d1af27f8b9ab05997ed44/html5/thumbnails/5.jpg)
Total Flange ImpedanceFlange Type Enamel Bellow Num. of
elementsFreq. [GHz] Impedance Q R/Q [Ω] Resistor
BPV-QD Yes Yes 90 1.21 633kΩ 315 2010 No
BPH-QF Yes Yes 39 1.28 1.03MΩ 400 2496 Long
QF-MBA Yes Yes 83 1.41 1.6MΩ 268 5985 Short
MBA-MBA Yes Yes 14 1.41 297kΩ 285 1040 Short
QF-QF No Yes 26 1.41 3.767MΩ 1828 2061 Short
QD-QD Yes No 99 1.57 17kΩ 55 317 No
QF-QF No No 20 1.61 588kΩ 980 600 No
BPH-QF Yes Yes 39 1.62 121kΩ 120 1014 Long
QD-QD No No 75 1.8 651kΩ 881 739 No
QD-QD Yes No 99 1.89 186kΩ 175 1070 No
No damping resistors included in simulations.
The ‘Resistor’ column states whether or not each element should have a resistor.
![Page 6: SPS flanges Simulations & Measurements Update Fritz Caspers and Jose E. Varela.](https://reader037.fdocuments.net/reader037/viewer/2022100403/5a4d1af27f8b9ab05997ed44/html5/thumbnails/6.jpg)
Outline
• Introduction• Impedance List Update• Damping Resistors in Simulations• Conclusions
![Page 7: SPS flanges Simulations & Measurements Update Fritz Caspers and Jose E. Varela.](https://reader037.fdocuments.net/reader037/viewer/2022100403/5a4d1af27f8b9ab05997ed44/html5/thumbnails/7.jpg)
Damping Resistor DC Measurement
A 4-wire DC measurement was taken on a long damping resistor as shown in the Figure.
The measured resistance was 160Ω.
A conductivity value of15.7 S/m for the
Nickel-Chrome layer was deduced from the measured
value.
![Page 8: SPS flanges Simulations & Measurements Update Fritz Caspers and Jose E. Varela.](https://reader037.fdocuments.net/reader037/viewer/2022100403/5a4d1af27f8b9ab05997ed44/html5/thumbnails/8.jpg)
Damping Resistor in SimulationsSimulation
no Resistor
Simulationwith
Resistor
Meas.no
Resistor
Meas.with
Resistor
f [GHz] 1.423 1.414
(-0.68%) 1.417 1.411(-0.42%)
Q0 1910 174 1930 186
The volume of the resistor represents around 1.5% of the total cavity volume.
6% rel. error
![Page 9: SPS flanges Simulations & Measurements Update Fritz Caspers and Jose E. Varela.](https://reader037.fdocuments.net/reader037/viewer/2022100403/5a4d1af27f8b9ab05997ed44/html5/thumbnails/9.jpg)
Outline
• Introduction• Impedance List Update• Damping Resistors in Simulations• Conclusions
![Page 10: SPS flanges Simulations & Measurements Update Fritz Caspers and Jose E. Varela.](https://reader037.fdocuments.net/reader037/viewer/2022100403/5a4d1af27f8b9ab05997ed44/html5/thumbnails/10.jpg)
Conclusions• All the elements in the original flange list have
been analysed.
• The impedance, Q and R/Q values have been provided for the bigger resonances.
• A ‘calibration’ of the conductivity value to be used in simulations for the Nickel-Chrome has been carried out.